2020
DOI: 10.1080/01495739.2020.1758263
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Wave propagation in an initially stressed magneto-thermoelastic medium with voids and microtemperatures

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Cited by 5 publications
(4 citation statements)
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“…In order to discuss the problem in greater detail and to find out the effects of various parameters considered in the medium on the physical fields, we now perform some numerical computations. For this purpose, the following values of relevant parameters are taken from Alshaikh [29]: The values of the microtemperature and magnetic parameters are taken from Kalkal et al [48]:…”
Section: Numerical Results and Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…In order to discuss the problem in greater detail and to find out the effects of various parameters considered in the medium on the physical fields, we now perform some numerical computations. For this purpose, the following values of relevant parameters are taken from Alshaikh [29]: The values of the microtemperature and magnetic parameters are taken from Kalkal et al [48]:…”
Section: Numerical Results and Discussionmentioning
confidence: 99%
“…\end{eqnarray*}$$The values of the microtemperature and magnetic parameters are taken from Kalkal et al. [48]: k1=0.0035kgms3,normalk2=0.0045kgms3,k3=0.0055kgms3normalK1,k4=0.0065kgnormalm3normals3,k5=0.0076kgnormalm3normals3,k6=0.0096kgnormalm3normals3,c1=0.15×109kgms2,μ0=0.7Hm1,ε0=0.3Hm1,H0=10Am1.$$\begin{eqnarray*} & &{k}_{1}=0.0035\hspace*{0.28em}\mathrm{kg}\hspace*{0.28em}{\mathrm{ms}}^{-3},\hspace*{0.28em}{\mathrm{k}}_{2}=0.0045\hspace*{0.28em}\mathrm{kg}\hspace*{0.28em}{\mathrm{ms}}^{-3},\hspace*{0.28em}{k}_{3}=0.0055\hspace*{0.28em}\mathrm{kg}\hspace*{0.28em}{\mathrm{ms}}^{-3}{\mathrm{K}}^{-1},\\ & & {k}_{4}=0.0065\hspace*{0.28em}\mathrm{kg}\hspace*{0.28em}{\mathrm{m}}^{3}{\mathrm{s}}^{-3},\hspace*{0.28em}{k}_{5}=0.0076\hspace*{0.28em}\mathrm{kg}\hspace*{0.28em}{\mathrm{m}}^{3}{\mathrm{s}}^{-3},\hspace*{0.28em}{k}_{6}=0.0096\hspace*{0.28em}\mathrm{kg}\hspace*{0.28em}{\mathrm{m}}^{3}{\mathrm{s}}^{-3},\\ & & {c}_{1}=0.15\ensuremath{\times{}}{10}^{-9}\hspace*{0.28em}\mathrm{kg}\hspace*{0.28em}{\mathrm{ms}}^{-2},\hspace*{0.28em}{\mu}_{0}=0.7{\mathrm{Hm}}^{-1},\hspace*{0.28em}{\varepsilon}_{0}=0.3{\mathrm{Hm}}^{-1},{H}_{0}=10\hspace*{0.28em}{\mathrm{Am}}^{-1}. \end{eqnarray*}$$Because …”
Section: Numerical Results and Discussionmentioning
confidence: 99%
“…In 2018, Ma et al [35] applied the fractional order theory and generalized thermoelastic theory, introduced the Lorentz force, and investigated the two-dimensional electromagnetic-thermal elasticity coupling problem. Recent research on the influence of an external magnetic field on the propagation of elastic waves by introducing the Lorentz force includes the work of Kalkal et al [36] in 2020, who considered prestresses and studied the propagation problem of plane waves in thermoelastic half-spaces with temperature and porosity. Kumar [37] utilized the Lord-Shulman generalized thermoelastic theory to derive a controlling equation for rotating orthogonal anisotropic magnetothermal elastic half-spaces and studied the reflection problem of elastic waves on stress-free adiabatic surfaces.…”
Section: Introductionmentioning
confidence: 99%
“…Othman et al [27] developed the mathematical model of thermoelasticity with the existence of initial stress, voids, and microtemperature. Kalkal et al [28] discussed wave nature in initially stressed thermoelastic problem with voids and microtemperature under magnetic field influence. Othman and Abd-Elaziz [29] observed effect of hall current and initial stress in porous thermoelastic condition with microtemperature.…”
Section: Introductionmentioning
confidence: 99%